Abstract:ABSTRACT. The experimental investigation of aerosol particles often requires special apparatus to ensure that the walls of the system interfere minimally with the measurements. Electrodynamic levitation offers an attractive approach because the particle, when suitably charged, is held away from the system walls by time-dependent electric fields. A new electrodynamic levitation system has been developed expressly for investigating aqueous particles in controlled gaseous environments. A cubic cell was used in co… Show more
“…Our ␣(HNO 3 ) values are slightly lower than those of Rudolf et al (2001), who put 0.3 as the lower limit based on binary condensation to small particles in an expansion chamber. But, the same arguments we have tentatively used to explain the empirical pressure dependence also lead us to expect ␣(HNO 3 ) to be relatively large over small particles at high supersaturations (Lamb et al 2004).…”
Section: The Accommodation Coefficientssupporting
confidence: 60%
“…The principles of electrodynamic levitation have been described in the literature (see Hartung and Avedisian 1992; Allison and Kendall 1996;Davis 1997), and details of our specific system are available elsewhere (Lamb et al 1996), so only a summary is presented here. The principles of electrodynamic levitation have been described in the literature (see Hartung and Avedisian 1992; Allison and Kendall 1996;Davis 1997), and details of our specific system are available elsewhere (Lamb et al 1996), so only a summary is presented here.…”
Section: A Experimental Apparatus and Proceduresmentioning
confidence: 99%
“…A moderate DC voltage (ϳ150 V) was applied to a stainless steel cylinder surrounding the glass tip, while the top end of the injector was grounded, causing the liquid to become polarized (Lamb et al 1996). The body of the droplet injector was constructed of 1/8" outside diameter stainless steel tubing and contained a small reservoir for the working fluid near the top.…”
Section: A Experimental Apparatus and Proceduresmentioning
Experiments were conducted with an electrodynamic levitation system to study the kinetics of droplet evaporation under chemically rich conditions. Single solution droplets of known composition (HNO 3 /H 2 O or H 2 SO 4 /HNO 3 /H 2 O) were introduced into an environmentally controlled cubic levitation cell. The gaseous environment was set intentionally out of equilibrium with the droplet properties, thus permitting the HNO 3 mass accommodation coefficient to be determined. Measurements were performed at room temperature and various pressures (200-1000 hPa). Droplet sizes (initial radii in the range 12-26 m) were measured versus time to high precision (Ϯ0.03 m) via Mie scattering and compared with sizes computed by different models for mass and heat transfer in the transition regime. The best agreement between the theoretical calculations and experimental results was obtained for an HNO 3 mass accommodation coefficient of 0.11 Ϯ 0.03 at atmospheric pressure, 0.17 Ϯ 0.05 at 500 hPa, and 0.33 Ϯ 0.08 at 200 hPa. The determination of the mass accommodation coefficient was not sensitive to the transport model used. The results show that droplet evaporation is strongly limited by HNO 3 and occurs in two stages, one characterized by rapid H 2 O mass transfer and the other by HNO 3 mass transfer. The presence of a nonvolatile solute (SO 2Ϫ 4 ) affects the activities of the volatile components (HNO 3 and H 2 O) and prevents complete evaporation of the solution droplets. These findings validate recent attempts to include the effects of soluble trace gases in cloud models, as long as suitable model parameters are used.
“…Our ␣(HNO 3 ) values are slightly lower than those of Rudolf et al (2001), who put 0.3 as the lower limit based on binary condensation to small particles in an expansion chamber. But, the same arguments we have tentatively used to explain the empirical pressure dependence also lead us to expect ␣(HNO 3 ) to be relatively large over small particles at high supersaturations (Lamb et al 2004).…”
Section: The Accommodation Coefficientssupporting
confidence: 60%
“…The principles of electrodynamic levitation have been described in the literature (see Hartung and Avedisian 1992; Allison and Kendall 1996;Davis 1997), and details of our specific system are available elsewhere (Lamb et al 1996), so only a summary is presented here. The principles of electrodynamic levitation have been described in the literature (see Hartung and Avedisian 1992; Allison and Kendall 1996;Davis 1997), and details of our specific system are available elsewhere (Lamb et al 1996), so only a summary is presented here.…”
Section: A Experimental Apparatus and Proceduresmentioning
confidence: 99%
“…A moderate DC voltage (ϳ150 V) was applied to a stainless steel cylinder surrounding the glass tip, while the top end of the injector was grounded, causing the liquid to become polarized (Lamb et al 1996). The body of the droplet injector was constructed of 1/8" outside diameter stainless steel tubing and contained a small reservoir for the working fluid near the top.…”
Section: A Experimental Apparatus and Proceduresmentioning
Experiments were conducted with an electrodynamic levitation system to study the kinetics of droplet evaporation under chemically rich conditions. Single solution droplets of known composition (HNO 3 /H 2 O or H 2 SO 4 /HNO 3 /H 2 O) were introduced into an environmentally controlled cubic levitation cell. The gaseous environment was set intentionally out of equilibrium with the droplet properties, thus permitting the HNO 3 mass accommodation coefficient to be determined. Measurements were performed at room temperature and various pressures (200-1000 hPa). Droplet sizes (initial radii in the range 12-26 m) were measured versus time to high precision (Ϯ0.03 m) via Mie scattering and compared with sizes computed by different models for mass and heat transfer in the transition regime. The best agreement between the theoretical calculations and experimental results was obtained for an HNO 3 mass accommodation coefficient of 0.11 Ϯ 0.03 at atmospheric pressure, 0.17 Ϯ 0.05 at 500 hPa, and 0.33 Ϯ 0.08 at 200 hPa. The determination of the mass accommodation coefficient was not sensitive to the transport model used. The results show that droplet evaporation is strongly limited by HNO 3 and occurs in two stages, one characterized by rapid H 2 O mass transfer and the other by HNO 3 mass transfer. The presence of a nonvolatile solute (SO 2Ϫ 4 ) affects the activities of the volatile components (HNO 3 and H 2 O) and prevents complete evaporation of the solution droplets. These findings validate recent attempts to include the effects of soluble trace gases in cloud models, as long as suitable model parameters are used.
“…[2][3][4][5][6][7][8] There is rapid development in the science of the phase transitions of atmospheric chemistry as well as a growing recognition of the importance of the condensed phase for diverse atmospheric problems. Laboratory work on cirrus and PSC cloud formation at low temperatures and salt crystallization at low relative humidities include 8 publications in 1999, 9-16 19 in 1997-1998, 17-35 14 in 1995-1996, [36][37][38][39][40][41][42][43][44][45][46][47][48][49] 18 in 1993-1994, 50-66 and 18 between 1977 and 1993. [67][68][69][70][71][72][73][74][75][76][77][78][79][80][81][82][83][84] Earlier work on salt crystallization is found in refs 85-88. In addition, there have been numerous papers describing field and modeling studies.…”
“…Thus, the drag force associated with a horizontal flow can be balanced with a dc field independently of the gravitational force using such a device. There is a renewed interest in the cubic device for studies in which flow through the chamber is needed (Lamb et al, 1996).…”
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.